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TheoremStatement: Literature-sourcedProof: AI-adaptedSession-authored (Fable 5 assisted)precheck passaudited 2026-08-02
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Young's theorem: total differentiability of the first partials forces equality of mixed partials

Statement

Let ff be defined on a disk UU about (a,b)(a,b), with fxf_x and fyf_y existing on UU. If fxf_x and fyf_y are totally differentiable at (a,b)(a,b), then both mixed partials exist there and fxy(a,b)=fyx(a,b)f_{xy}(a,b)=f_{yx}(a,b).

Facts & Assumptions

Given: The hypotheses of the statement.

[L1]

Total differentiability supplies a linear approximation with an error that is little-oh of the Euclidean increment (The total (Fréchet) derivative Df(a)Df(a) as the linear first-order approximation with o(h2)o(\|h\|_2) remainder).

[L2]

A total derivative is linear. Restricting its defining expansion to a coordinate axis shows directly that its corresponding coordinate coefficient is the partial derivative in that coordinate (The total (Fréchet) derivative Df(a)Df(a) as the linear first-order approximation with o(h2)o(\|h\|_2) remainder).

Proof

technique · direct
1.1

By [L1] and [L2], write Dfx(a,b)(s,t)=As+BtDf_x(a,b)(s,t)=As+Bt and Dfy(a,b)(s,t)=Cs+DtDf_y(a,b)(s,t)=Cs+Dt.

L1L2givenalgebra

fx(a+s,b+t)=fx(a,b)+As+Bt+o ⁣(s2+t2)f_x(a+s,b+t)=f_x(a,b)+As+Bt+o\!\left(\sqrt{s^2+t^2}\right)

and analogously fy(a+s,b+t)=fy(a,b)+Cs+Dt+o ⁣(s2+t2)f_y(a+s,b+t)=f_y(a,b)+Cs+Dt+o\!\left(\sqrt{s^2+t^2}\right). Restricting the first expansion to s=0s=0 and the second to t=0t=0 shows that B=fxy(a,b)B=f_{xy}(a,b) and C=fyx(a,b)C=f_{yx}(a,b); in particular both mixed partials exist.

2.1

By [L3], for small nonzero hh, define the following rectangular difference.

step 1.1L3algebrachoose

Δh:=f(a+h,b+h)f(a+h,b)f(a,b+h)+f(a,b).\Delta_h:=f(a+h,b+h)-f(a+h,b)-f(a,b+h)+f(a,b).

Apply the mean-value theorem to xf(x,b+h)f(x,b)x\mapsto f(x,b+h)-f(x,b) on the interval with endpoints a,a+ha,a+h. For some θh\theta_h between 00 and 11,

Δh=h(fx(a+θhh,b+h)fx(a+θhh,b))=Bh2+o(h2),\Delta_h=h\bigl(f_x(a+\theta_hh,b+h)-f_x(a+\theta_hh,b)\bigr)=Bh^2+o(h^2),

where the last equality is the first expansion of step 1.1 at (θhh,h)(\theta_hh,h) and (θhh,0)(\theta_hh,0).

2.2

Apply [L3] instead to yf(a+h,y)f(a,y)y\mapsto f(a+h,y)-f(a,y) on the interval with endpoints b,b+hb,b+h.

step 1.1L3algebrachoose

For some ηh\eta_h between 00 and 11,

Δh=h(fy(a+h,b+ηhh)fy(a,b+ηhh))=Ch2+o(h2),\Delta_h=h\bigl(f_y(a+h,b+\eta_hh)-f_y(a,b+\eta_hh)\bigr)=Ch^2+o(h^2),

by the second expansion of step 1.1 at (h,ηhh)(h,\eta_hh) and (0,ηhh)(0,\eta_hh).

3.1

Steps 2.1 and 2.2 give (BC)h2=o(h2)(B-C)h^2=o(h^2). Divide by h2h^2 and let h0h\to0 to obtain B=CB=C, hence fxy(a,b)=fyx(a,b)f_{xy}(a,b)=f_{yx}(a,b).

step 1.1step 2.1step 2.2algebra

Depends on

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